The parameters \(f^p_{Tq}\)  can be found in Ref. [1]}.
Fig. REF  shows the results for DM-nucleon scattering. It is clear that the choice of \(\sin \alpha =0.1\)  is enough to escape current XENON1T limit, but most range is in the reach of LZ. Since \(\sigma ^\text{SI}\)  is sensitive to \(\sin \alpha \) , we further derive the corresponding experimental limits. We find current XENON1T limit on \(\sin \alpha \)  is actually less stringent than collider limit in Ref. [2]}. Meanwhile, if no signal is observed at LZ, then \(\sin \alpha \lesssim 0.05\)  should be satisfied.
